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Breaking time for the quantum chaotic attractor.

A Iomin1, G M Zaslavsky

  • 1Department of Physics, Technion, Haifa 32000, Israel.

Physical Review. E, Statistical, Nonlinear, and Soft Matter Physics
|March 15, 2003
PubMed
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This study examines quantum dissipative systems where classical limits show chaotic attractors. Researchers found that the breaking time of classical-quantum correspondence can be arbitrarily large for dying attractors.

Area of Science:

  • Quantum physics
  • Chaos theory
  • Statistical mechanics

Background:

  • Classical-quantum correspondence is crucial for understanding physical systems.
  • Dissipative systems and chaotic attractors present unique challenges in quantum mechanics.
  • The breaking time of classical-quantum correspondence indicates the limits of classical descriptions.

Purpose of the Study:

  • To investigate the breaking time of classical-quantum correspondence in a quantum dissipative system.
  • To analyze a model exhibiting a chaotic attractor in its classical limit.
  • To explore the influence of dissipation on the classical-quantum correspondence.

Main Methods:

  • A theoretical model of a periodically kicked harmonic oscillator with dissipation was developed.

Related Experiment Videos

  • The model was analyzed in the regime where the classical limit corresponds to a chaotic attractor.
  • The breaking time, tau(Planck), of classical-quantum correspondence was mathematically derived.
  • Main Results:

    • The study obtained the breaking time, tau(Planck), for classical-quantum correspondence.
    • It was demonstrated that tau(Planck) can be arbitrarily large in the limit of a dying attractor.
    • The model serves as an analog for the dissipative kicked Harper model.

    Conclusions:

    • The breaking time of classical-quantum correspondence in dissipative chaotic systems is sensitive to attractor properties.
    • The concept of a 'dying attractor' allows for an extended validity of classical descriptions in quantum systems.
    • This research provides insights into the boundary between classical and quantum physics in dissipative chaotic regimes.